öÕÒÎÁÌ üËÓÐÅÒÉÍÅÎÔÁÌØÎÏÊ É ôÅÏÒÅÔÉÞÅÓËÏÊ æÉÚÉËÉ
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ïÂÝÁÑ ÉÎÆÏÒÍÁÃÉÑ Ï ÖÕÒÎÁÌÅ
úÏÌÏÔÙÅ ÓÔÒÁÎÉÃÙ
áÄÒÅÓÁ ÒÅÄÁËÃÉÉ
óÏÄÅÒÖÁÎÉÅ ÖÕÒÎÁÌÁ
óÏÏÂÝÅÎÉÑ ÒÅÄÁËÃÉÉ
ðÒÁ×ÉÌÁ ÄÌÑ Á×ÔÏÒÏ×
úÁÇÒÕÚÉÔØ ÓÔÁÔØÀ
ðÒÏ×ÅÒÉÔØ ÓÔÁÔÕÓ ÓÔÁÔØÉ


öüôæ, ôÏÍ 133, ÷ÙÐ. 3, íÁÒÔ 2008
(áÎÇÌÉÊÓËÉÊ ÐÅÒÅ×ÏÄ - JETP, Vol. 106, No 3, March 2008 ÄÏÓÔÕÐÅÎ on-line ÎÁ www.springer.com )


áÔÏÍÙ, ÍÏÌÅËÕÌÙ, ÏÐÔÉËÁ

ó÷ñúáîîùå íîïçï÷ïìîï÷ùå ÷úáéíïäåêóô÷éñ ÷ áðåòéïäéþåóëé ðïìñòéúï÷áîîùè îåìéîåêîï-ïðôéþåóëéè ëòéóôáììáè
  483
óéóôåíá õòá÷îåîéê íáëó÷åììá - ûòåäéîçåòá äìñ úáäáþé ï ÷úáéíïäåêóô÷éé âïúå-üêîûôåêîï÷óëïçï ëïîäåîóáôá òáúòåöåîîïçï çáúá ó üìåëôòïíáçîéôîùí ðïìåí
  495
QUANTUM TELEPORTATION THROUGH AN ENTANGLED STATE COMPOSED OF DISPLACED VACUUM AND SINGLE-PHOTON STATES
  505
ïâÿåíîïå æòåîåìå÷ï ïôòáöåîéå üìåëôòïíáçîéôîùè ÷ïìî ÷ ôòåèíåòîï îåïäîïòïäîùè óòåäáè
  513
çåîåòáãéñ óòåäîåçï éîæòáëòáóîïçï éúìõþåîéñ ÷ ðïìõðòï÷ïäîéëï÷ùè ìáúåòáè âìéöîåê éîæòáëòáóîïê ïâìáóôé îá îéúëïòáúíåòîùè çåôåòïóôòõëôõòáè
  522
ä÷éöåîéå äéóóéðáôé÷îùè óïìéôïîï÷ ÷ ìáúåòå ó ðìá÷îïê ðïðåòåþîïê îåïäîïòïäîïóôøà
  532

ñÄÒÁ, ÞÁÓÔÉÃÙ, ÐÏÌÑ, ÇÒÁ×ÉÔÁÃÉÑ É ÁÓÔÒÏÆÉÚÉËÁ

FINAL-STATE RADIATION AND THE POSSIBILITY TO TEST A PION-PHOTON INTERACTION MODEL NEAR THE TWO-PION THRESHOLD
  544
IS ASTRONOMY POSSIBLE WITH NEUTRAL ULTRAHIGH ENERGY COSMIC RAY PARTICLES EXISTING IN THE STANDARD MODEL?
  556
INVERSE BREMSSTRAHLUNG CONTRIBUTION TO DRELL-YAN-LIKE PROCESSES
  564

ðÏÒÑÄÏË, ÂÅÓÐÏÒÑÄÏË É ÆÁÚÏ×ÙÅ ÐÅÒÅÈÏÄÙ × ËÏÎÄÅÎÓÉÒÏ×ÁÎÎÙÈ ÓÒÅÄÁÈ

ðïóôòïåîéå äéîáíéþåóëïê íáôòéãù çðõ-ëòéóôáììá îá ïóîï÷å äáîîùè ï æïîïîáè ÷ ôïþëáè óéííåôòéé úïîù âòéììàüîá é ï íïäõìñè õðòõçïóôé
  571
óáíïïòçáîéúáãéñ îáîïïóôòï÷ëï÷ çåòíáîéñ ðòé éíðõìøóîïí ïâìõþåîéé ðõþëïí îéúëïüîåòçåôéþåóëéè éïîï÷ ÷ ðòïãåóóå çåôåòïüðéôáëóéé óôòõëôõò Ge/Si(100)
  593
÷ìéñîéå éúïôïðéþåóëïçï óïóôá÷á é íéëòïóôòõëôõòù îá ëòéóôáììéþåóëïå é íáçîéôîïå æáúï÷ïå óïóôïñîéå ÷ R0.5Sr0.5MnO3
  605
îåüíðéòéþåóëéê òáóþåô óåçîåôïüìåëôòéþåóëïçï æáúï÷ïçï ðåòåèïäá ÷ îåõðïòñäïþåîîùè é õðïòñäïþåîîùè ô÷åòäùè òáóô÷ïòáè PbSc0.5Ta0.5O3 ¿é PbSc0.5Nb0.5O3 ó éóðïìøúï÷áîéåí íïäåìøîïçï çáíéìøôïîéáîá
  622
óòá÷îéôåìøîùå éóóìåäï÷áîéñ ðïçìïýåîéñ íéëòï÷ïìîï÷ïçï éúìõþåîéñ ÷ óéîçìåôîùè ðáòáíáçîåôéëáè HoVO4 é HoBa2Cu3Ox ÷ óéìøîùè éíðõìøóîùè íáçîéôîùè ðïìñè
  632

üÌÅËÔÒÏÎÎÙÅ Ó×ÏÊÓÔ×Á Ô×ÅÒÄÙÈ ÔÅÌ

íïäéæéëáãéñ ìïëáìéúï÷áîîùè é òåúïîáîóîùè óïóôïñîéê îá îåóéííåôòéþîùè ëïòïôëïäåêóô÷õàýéè äåæåëôáè ðòé çéäòïóôáôéþåóëïí óöáôéé
  646
üææåëô ä÷ïêîïçï òåúïîáîóá ðòé ëïíâéîáãéïîîïí òáóóåñîéé ó÷åôá ÷ îáîïçòáæéôîùè ðìåîëáè
  654
ïðôéþåóëéå ó÷ïêóô÷á äïðéòï÷áîîùè çòáæåîï÷ùè óìïå÷
  663
MOTT-HUBBARD TRANSITION AND ANDERSON LOCALIZATION: A GENERALIZED DYNAMICAL MEAN-FIELD THEORY APPROACH
  670

óÔÁÔÉÓÔÉÞÅÓËÁÑ, ÎÅÌÉÎÅÊÎÁÑ ÆÉÚÉËÁ, ÆÉÚÉËÁ <<ÍÑÇËÏÊ ÍÁÔÅÒÉÉ>>

äéîáíéëá óáíïðïäïâîùè ó÷åôï÷ùè éíðõìøóï÷ ðòåäåìøîïê äìéôåìøîïóôé é üîåòçéé ÷ ÷ïìïëïîîïí ìáúåòå
  687
REPTATION AND DIFFUSIVE MODES OF MOTION OF LINEAR MACROMOLECULES
  696
ï òåìáëóáãéé óòåäù ðïóìå åå ÷ïúâõöäåîéñ ïäéîïþîùíé âùóôòùíé ôñöåìùíé éïîáíé
  701
 
óÏÏÂÝÉÔØ Ï ÔÅÈÎÉÞÅÓËÉÈ ÐÒÏÂÌÅÍÁÈ